US 7441416 B2
Multi-flame burner wherein each flame is separated with respect to the neighboring flame by at least one separating tube made of a heat resistant material, for example, quartz glass or ceramic material. The burner also has a plurality of co-axial pipes, preferably made of a metallic material. The cross section of the upper end of the separating tube can be modified in order to increase the deposition rate of the burner. Methods for manufacturing optical fibre preforms by vapour deposition using the multi-flame deposition burners.
1. A method for manufacturing an optical preform by directing a flow of fine glass particles from a deposition burner onto a rotating elongated target preform, said method comprising the steps of:
(a) feeding said burner with a flow of a glass precursor material via a first plurality of ducts and directing said flow of glass precursor material toward said target preform;
(b) feeding said burner with a first flow of combustible gas and a first flow of combustion sustaining gas via said first plurality of ducts in order to generate an inner flame surrounding said flow of glass precursor material;
(c) feeding said burner with a second flow of combustible gas and a second flow of combustion sustaining gas via a second plurality of ducts in order to generate an outer flame surrounding said inner flame;
(d) reacting said glass precursor material in the presence of said flames, thus forming a flow of fine glass particles directed toward said target preform; and
(e) confining and separating said inner flame from said outer flame with an elongated hollow separating element made of a heat resistant material that surrounds said inner flame and that does not form a part of a duct for the passage of any gas or glass precursor material.
2. A method according to
3. A method according to
4. A method according to
5. A method according to
This application is a national phase application based on PCT/EP01/14016, filed Nov. 30, 2001, the content of which is incorporated herein by reference, and claims the priority of European Patent Application No. 00127851.4, filed Dec. 19, 2000, and claims the benefit of U.S. Provisional Application No. 60/256,942, filed Dec. 21, 2000.
1. Field of the Invention
The present invention relates to a burner for manufacturing an optical fiber preform used to make optical glass fibers and to a method for producing said optical, preforms.
In particular, the present invention relates to a multi-flame deposition burner suitable for manufacturing optical preforms in an efficient and stable manner at high fabrication rate and to a method for producing an optical preform by using said burner.
2. Background Art
Glass fibers for optical communication are made from high purity, silica-based glass fibers drawn from glass preforms, which preforms are produced according to various glass deposition techniques.
Some of these deposition techniques, including vapor axial deposition (VAD) and outside vapor deposition (OVD), are based on flame combustion wherein reactants (i.e. silica precursors, such as SiCl4, optionally together with dopants materials, such as GeCl4, for suitably modifying the refractive index of the glass) are fed together with combusting gases through a deposition burner which directs a high temperature flow of forming fine glass particles onto a rotating growing target preform.
According to the VAD deposition technique, the growth of the preform takes place in an axial direction. Thus, the deposition burner(s) is typically maintained in a substantially fixed position, while the rotating preform is slowly moved upwardly (or downwardly) with respect to the burner, in order to cause the axial growth of the preform. Alternatively, the rotating preform can be maintained in a substantially fixed position, while the deposition burner is slowly moved downwardly (or upwardly) with respect to the preform.
Differently from the VAD technique, in the OVD technique the growth of the preform takes place in a radial direction. In this case, a rotating target (e.g. a quartz glass rod) is generally positioned in a fixed horizontal or vertical position and the deposition burner is repeatedly passed along the surface of the growing preform for causing the radial growth of the same.
Independently from the applied deposition technique, a porous glass preform is thus fabricated, which is then consolidated to form a solid glass preform apt for being subsequently drawn into an optical fiber.
Typically, an optical preform comprises a central portion (core) and an outer portion (cladding), the core and the cladding differing in their respective chemical composition and having thus different refractive indexes. As in the optical fibers, the cladding portion forms the majority of the preform. The preform is typically manufactured by producing and consolidating a first preform comprising the core and a first portion of the cladding. An overcladding layer is then deposited onto said first preform, thus obtaining a porous preform, which is then consolidated into the final preform.
In general, conventional burners for manufacturing optical preforms are made up of a plurality of co-axial pipes through which the glass precursor materials (i.e. silica precursors, such as SiCl4, optionally together with dopants materials, such as GeCl4), the combusting gases (e.g. oxygen and hydrogen or methane) and, optionally, some inert gas (e.g. argon or helium) are fed. Typically, the glass precursor material is fed through the central pipe of the burner, while other gases are fed through the annular openings formed by the concentrically disposed pipes.
Examples of such conventional burners are disclosed, for instance, in U.S. Pat. Nos. 4,345,928, 4,465,708, 4,474,593, 4,661,140, and 4,810,189.
“Multi-flame” burners, generating a plurality of independent flames disposed concentrically one to each other, are also disclosed. For instance, U.S. Pat. No. 4,801,322 discloses a multi-flame burner wherein the inner flame, including a glass precursor material, is positioned rearwardly of the outer flame. As mentioned in said patent, the outer flame allows to increase the flame length with consequent size increase of the synthesised glass particles.
U.S. Pat. No. 4,826,520 discloses a modified multi-flame burner for producing doped optical preforms wherein a central pipe, through which a doping reactant (GeCl4) is fed, is spaced forwardly with respect to the other pipes forming the inner flame, in order to reduce the staying time of the doping material inside the flame.
Although few prior art documents disclose burner having pipes made from a heat resistant metallic cylindrical material (e.g. U.S. Pat. No. 4,661,140), the pipes of conventional prior art burners are generally and more desirably made from quartz glass or ceramic materials, as disclosed for instance in U.S. Pat. No. 4,345,928 (col. 8, lines 52-55), U.S. Pat. No. 4,474,593 (col. 2, lines 16-19), U.S. Pat. No. 4,465,708 (col. 1, lines 58-61), U.S. Pat. No. 4,801,322 (col. 26, lines 32-40) and U.S. Pat. No. 4,810,189 (col. 4, lines 66-68).
As a matter of fact, quartz or ceramic materials are more heat resistant than metallic materials to high temperatures and may thus more easily withstand the typical temperature developed by the flame in the burner. In any case, the possible use of heat resistant metallic pipes in conventional deposition burner is necessarily limited to the single-flame type burners (such as the one disclosed in U.S. Pat. No. 4,661,140). In these burners, all the co-axial pipes through which reactants/inert gases flow have in fact substantially the same length; the overheating of said pipes is thus avoided by maintaining the flame sufficiently spaced apart from the tips of the pipes.
However, as observed by the Applicant, in the multi-flame burners of the prior art, such as the one disclosed in U.S. Pat. No. 4,801,322, problems may arise in using metallic materials for manufacturing the pipes of the burner. In fact, as disclosed in the above cited patent, the pipes generating outer flame are longer than the pipes generating the inner flame, in order to obtain the rearward spacing of the inner flame with respect to the outer flame. Thus, the inner surface of the pipes forming the outer flame is subjected to the heat generated by the inner flame. While the typical temperature of a flame is of about 2500-3000° C., the surface of the pipes exposed to the flame may reach a temperature of several hundreds degrees, typically of about 600-800° C. As it is apparent that a pipe made from a metallic material can not withstand the heat generated by such a flame, it is therefore necessary, as mentioned in the above cited patent, to use a burner with quartz glass pipes. This problem is much more evident for burners specifically designed for the outer cladding deposition, which produce larger flames and accordingly higher amount of heat.
The Applicant has however observed that the use of quartz glass or ceramic materials for producing a burner results in a number of drawbacks. In particular, the concentricity of glass pipes is rather cumbersome to obtain and particular attention shall be paid to the relative alignment of the co-axial pipes. In addition, a burner containing a plurality of glass pipes shall be handled with care for avoiding possible damages of the pipes.
The Applicant has now found that in a multi-flame burner, comprising at least an inner section comprising a first plurality of ducts for generating an inner flame and at least an outer section comprising a second plurality of ducts for generating an outer flame surrounding said inner flame, said inner flame can be advantageously confined and separated from the outer flame by disposing a separating tube made of a heat resistant material, in particular of quartz glass or ceramic material (e.g. alumina), between said inner and said outer section.
According to such a burner design, the pipes forming the ducts of the multi-flame burner may thus advantageously be made from a metallic material, e.g. stainless steel.
In addition, as observed by the Applicant, while the burners for depositing the core and the inner cladding of the preform are generally of reduced dimensions, the burner used for depositing the overcladding, in particular for large dimensions preforms, shall be relatively larger, in order to allow the generation of higher flow rates which are necessary for increasing the amount of deposited material, maintaining at the same time the velocity of the gases relatively low.
The Applicant has thus observed that, particularly for overcladding deposition and especially when manufacturing large diameter optical preforms, the deposition rate of the process can be increased by suitably modifying the geometry of deposition burner in order to redistribute the flow of fine glass particles impacting onto the target preform. In particular, it has been observed that the shape of said flow can be advantageously modified in its terminal portion before impacting onto the target preform, by increasing the dimension of said flow in a direction substantially perpendicular to the longitudinal axis of said target preform.
The modification of the geometry of the flow of glass particles is particularly easy and effective when applied onto a multi-flame burner with a. single flame-separating tube according to the present invention.
One aspect of the present invention thus relates to a multi-flame burner for manufacturing an optical fiber preform comprising:
Preferably, said first plurality of ducts disposed in the inner section of the burner is made from a metallic material. Advantageously, also the second plurality of ducts disposed in the outer section of the burner is made from a metallic material.
According to a preferred embodiment, a second elongated hollow element made of heat resistant material is disposed to surround the outer section of the burner for containing the outer flame.
Preferably, said inner and said outer section of the burner are of substantial circular form. Advantageously, said inner and said outer section of the burner are formed from a plurality of co-axial pipes made of metallic material.
According to a preferred embodiment, the separating element is an elongated pipe of a heat resistant material, preferably of quartz glass or ceramic material, such as alumina.
Preferably, said separating elongated hollow element extends for a length such as to surround the majority of the length of the reaction zone of the glass precursor material.
Preferably, said separating elongated hollow element extends for a length of about at least 80 mm from the tips of the ducts forming the inner section of the burner. Preferably, said separating elongated hollow element extends for a length of less than about 150 mm from the tips of the ducts forming the inner section of the burner.
According to an embodiment, the length of the ducts forming the inner and the outer section of the burner are substantially the same.
Advantageously, the inner section of the burner is spaced rearwardly of the outer section. Preferably, the pipes forming the outer section are from about 30 mm to about 80 mm longer than the pipes forming the inner section of the burner, more preferably from about 40 mm to about 65 mm.
According to a preferred embodiment, the elongated hollow element separating the two portion of the burner has an upper terminal portion which is formed into an elliptical cross-section.
A further aspect of the present invention relates to a method for manufacturing an optical preform by directing a flow of fine glass particles from a deposition burner onto a rotating elongated target preform, said method comprising the steps of:
A further aspect of the present invention relates to a method for manufacturing an optical preform by directing a flow of fine glass particles from a multi-flame deposition burner comprising a plurality of ducts onto a rotating elongated target preform by using a multi-flame deposition burner as above described.
The burner of
Openings 101 a-103 a define the inner section of the burner, while openings 4 a-7 a define the outer section. The central opening 101 a is delimited by the walls of a metal pipe 101, while the other annular openings are delimited by the respective outer and inner walls of metal pipes 101 to 108. The length of the metal pipes can be substantially the same, as shown in detail in
The metal pipes are preferably made from an easily machinable and heat/corrosion resistant stainless steel. An example of a suitable metal material is AISI (American Institute Steel and Iron) 316L, which is a stainless steel comprising about 0.03% C about 16-18% of Cr, about 11.5%-14.5% of Ni, about 2% of Mn and about 2.5%-3% of Mo.
Typically, the inner pipe 101 has an inner diameter of from about 6 mm to about 8 mm and a thickness of from about 0.5 mm to about 2 mm.
The other metal pipes, having preferably a thickness comprised from about 0.5 mm to about 2.5 mm, are then arranged coaxially one to each other to form openings 102 a-107 a having widths of from about 1 mm to about 3.5 mm, depending on the relative diameter of the pipe and flow rate of gas through the aperture.
In particular, the width of each opening is selected according to the amount and kind of gas which is flown through said opening and to the relative radial position of said opening. For instance, in a burner particularly designed for the outer cladding deposition, openings through which inert gas is flown are dimensioned so to obtain an exit velocity of the gas of from about 0.1 and about 2 m/s. Said annular openings may thus have a width of from about 1 mm to about 1.5 mm. On the other side, openings through which combustion gases are flown are dimensioned so to obtain an exit velocity of the gas of from about 2 and about 10 m/s. Said annular openings may thus have a width of from about 2 mm to about 3.5 mm.
A separating tube 109 made from a heat resistant material, is disposed into the annular housing between pipes 103 and 104, said tube extending for a certain length farther from the tips of the pipes of the inner portion of the burner, as shown in
Tube 109 allows both to confine the inner flame for a certain length and to physically separate it from the outer flame. In addition, when the pipes forming the outer section of the burner are longer than the pipes forming the inner section, said tube 109 avoids a direct contact of the inner flame with the surface of the innermost metal pipe of the outer section.
A second tube 110, also made from heat resistant material, can be disposed externally to the metal pipe 108, extending for a certain length farther from the tips of the pipes of the outer portion of the burner, as shown in
For the purposes of the present invention, the term “heat resistant material” is intended to refer to a material capable of resisting to temperatures typically present in a deposition burner during a preform manufacturing process, without undergoing to physical or chemical damages.
The heat resistant material of tubes 109 and 110 is for instance quartz glass or ceramic material, such as alumina. Preferably quartz, in particular high purity quartz, is employed.
Preferably, the separating tube 109 extends for a length such to surround the majority of the length of the reaction zone where the glass precursor material reacts to form the glass particles.
Methods for approximately calculating the extension of the reaction zone are well known and widely discussed in several reference books, such as K. K. Kuo, “Principles of Combustion”, Wiley and Sons Ed., New York. 1986, p. 370.
An example of such calculation is given hereinafter, with specific reference to a burner having the following configuration:
As an approximation, it is assumed that all the hydrogen instantaneously reacts with oxygen at the outlet of the ducts. A flow of water and oxygen, surrounding the central flow of silicon tetrachloride, is thus formed. The glass precursor material reacts with the formed water to form silica, according to the following reaction:
The length of the reaction zone can thus be calculated by applying the following relationship:
The separating tube may thus preferably have a length substantially equivalent to the calculated length of the reaction zone. Said tube may be up to about 50-60% longer than said calculated length. Longer lengths of the tube, e.g. 60% or more with respect to the calculated length of the reaction zone (in particular more than about 70%), while not substantially increasing the deposition rate of the burner, may conversely negatively affect the deposition process. For instance, if the separating tube is excessively long and the burner is kept too close to the target preform, the deposited soot can be subjected to undesirable local overheating, with consequent formation of cracks in the soot. On the other side, if the burner is too spaced from the preform in order to avoid the above overheating drawbacks, an irregular growth of the silica glass particles may occur, with consequent reduction of the deposition rate.
Thus, particularly for overcladding burners, depending from the dimensions of the ducts and the flow rate and velocity of the gases flowing therethrough, the Applicant has determined that the separating tube 109 should preferably extend for at least about 80 mm from the tips of the pipes of the inner section of the burner. The length of the tube should however preferably not exceed about 150 mm. Preferably, said length is from about 90 to about 130 mm. When the pipes forming the inner section of the burner are spaced rearwardly with respect to the pipes of the outer section, the separating tube preferably extends for at least about 40 mm from the tips of the pipes of the outer section, more preferably for at least 50 mm, up to about e.g. 100 mm, preferably 85 mm.
The outer tube 110 preferably extends for about 150 mm to about 220 mm from the tips of the pipes of the outer section.
Advantageously, the metallic coaxial pipes are first assembled together to form the burner, leaving a suitable annular clearance between two neighbouring pipes, said clearance being apt to receive the separating quartz tube 109. The separating tube 109 can thus be inserted into and (if necessary) removed from said annular clearance with a rather simple operation. Similarly, the outer glass tube 110 can be fitted on (and removed from) the outer surface of the outer metal pipe (suitably adapted for receiving said glass tube), after the metal pipes of the burner have been assembled together.
With the above construction, the size and concentricity of the metal co-axial pipes forming the burner can be controlled much more easier than in conventional multi-flame burners where the co-axial pipes are made from quartz glass. In addition, the manufacturing, handling and maintenance of such burner can be performed in a rather simple manner, without the risk of breaking the pipes. Only a single glass tube is used for confining the inner flame and separating it from the outer one, which tube can be easily fitted into the burner after the whole burner has been assembled and (if necessary) removed from it, for instance in case of accidental breakage of the same.
Although the heat resistant materials from which tubes 109 and 110 are made can withstand rather easily the typical temperatures developed by the flames of the burner, it may be desirable to reduce the heat transmitted from the flames towards the surfaces of the heat resistant tubes.
Thus, in order to lower the heat transmitted from the flames towards the surfaces of heat resistant tubes 109 and 110, a gas is preferably allowed to flow along the internal and/or external walls of tube 109 and preferably also along the internal wall of tube 110, to create a boundary layer on the respective surfaces of the tubes. The presence of such boundary layer may in fact contribute to dissipate the heat generated by the flames, thus avoiding possible overheating of the tubes. Preferably, said boundary layer is formed by a laminar flow of gas. To this end, any gas capable of forming said boundary layer at the relevant flow rates applied during the deposition operations can be employed. Preferably, oxygen or inert gases, such as argon, helium or nitrogen, are employed.
Typically, the central duct 101 of a multi-flame burner according to the present invention is fed with a flow of glass precursor material, optionally admixed with a high thermal diffusivity gas. In the present description, the term glass precursor material is intended to refer to any suitable material capable of reacting in the presence of an oxidizing flame to form glass (pure silica) or doped glass particles. Preferably, silicon tetrachloride (SiCl4) can be used. Alternatively, other silicon containing reactants can be used, such as SiHCl3, SiH2Cl2, SiH3Cl or SiH4. In addition chlorine-free silicon containing reactants can be used, such as the siloxane compounds disclosed in U.S. Pat. No. 5,043,002, e.g. octamethylcyclotetrasiloxane, or the organosilicone compounds disclosed in European Patent Application Publ. No. EP 1,016,635, e.g. hexamethyldisilane.
A preferred glass precursor material capable of forming doped glass particles under the reaction conditions of a flame burner according to the invention is GeCl4) Germanium tetrachloride. Alternative dopant materials are POCl3 or BBr3.
Mixtures of the above glass precursor materials (e.g. SiCl4 and GeCl4) in variable proportion can be used to suitably modify the refractive index of the produced preform.
As the above glass precursor materials are generally liquid at ambient temperature, they may be fed as liquids to the metal pipes of the burner or they may be preferably vaporized in advance, so that high temperature vapors of the glass precursor material are flown through the central pipe of the burner.
As previously mentioned it may be advantageous, in particular for relatively large dimension burners (e.g. cladding burners), to add a predetermined amount of a high thermal diffusivity gas to the flow of glass precursor material, in order to increase the heat transfer from the flame towards the inner core of said flow.
The thermal diffusivity of a gas is defined as the ratio of the thermal conductivity to the heat capacity. It measures the ability of a material to conduct thermal energy relative to its ability to store thermal energy. Typical values of thermal diffusivity of gases can be found on a number of reference books, such as R. B. Bird, “Transport Phenomena”, Wiley & Sons, New York 1960, or F. P. Incropera, D. P. DeWitt, “Fundamentals of heat and mass Transfer”, Wiley and Sons; 3rd edition, New York, 1996.
For the purposes of the present invention, a high thermal diffusivity gas is a gas having a thermal diffusivity of at least 3.0·10−5 m2/s or higher, e.g. up to about 2.0·10−4 m2/s (values at 400° K.). Examples of suitable high thermal diffusivity gases are oxygen, nitrogen, argon, helium or hydrogen, having a thermal diffusivity at 400° K. of 3.6·10−5 m2/s, 3.7·10−5 m2/s, 3.8·10−5 m2/s, 3.0·10−4. m2/s and 2.3·10−4 m2/s, respectively.
As the thermal diffusivity of a gas depends, further from its specific thermal diffusivity coefficient, also from the mass fraction of the added gas, it is preferable to use gases with a higher molecular weight, in order to reduce the volume fraction of added gas (or, alternatively, using the same volume fraction of gas, increase its mass fraction). Oxygen is thus preferred for its higher molecular weight and for its relatively high coefficient of thermal diffusivity.
Said high thermal diffusivity gas should preferably be added to the flow of glass precursor material in an amount such that the overall thermal diffusivity of the so obtained mixture is about 50% higher than the thermal diffusivity of the glass precursor material. In particular, when silicon tetrachloride is used, the thermal diffusivity of the mixture should preferably be higher than about 4.0·10−6 m2/s at 400° K. Preferably, the thermal diffusivity of the mixture is comprised between 4.0·10−6 m2/s and 5.5·10−6 m2/s at 400° K.
The high thermal diffusivity gas is preferably admixed in a volume fraction of from about 0.05 to about 0.5 parts with respect to the total volume of the mixture, preferably of from about 0.1 to about 0.4 parts, depending also from the thermal diffusivity of the glass precursor material (e.g. 2.84·10−6 m2/s at 400° K. for SiCl4).
A combustible gas and a combustion sustaining gas are then flown through the annular ducts of the burner formed by the co-axial metal pipes, optionally together with an inert gas. Examples of suitable combustible gas are hydrogen or hydrocarbons, such as methane. Oxygen is typically used as the combustion sustaining gas.
If desired, an inert gas may be flown through the annular ducts, either alone or admixed with the above combustible gas or combustion sustaining gas. For instance, an inert gas may be flown through an annular duct disposed between a first annular duct dedicated to the inlet of a combustible gas and a second annular duct dedicated to the inlet of a combustion sustaining gas. This allows a physical separation of the two flows of combustible gas and of combustion sustaining gas, thus displacing the flame away from the tips of the metal pipes and avoiding possible overheating of the same. Similarly, the flame can be displaced away from the tips of the metal pipes by suitably increasing the inlet speed of the combustible gas and of combustion sustaining gas. Examples of suitable inert gases are argon, helium, nitrogen.
With specific reference to
Said excess of oxygen allows to obtain a convergent flame and to create an oxygen boundary layer on the inner surface of the quartz tube 109, for reducing the heat transferred onto the quartz tube. For determining the excess of oxygen in the inner flame, also the possible reaction of said oxygen with the hydrogen flowing from the outer section of the burner shall be taken into account. In order to effectively create said boundary layer, the Applicant has observed that the inlet speed of the oxygen gas into the burner should preferably be of at least 3.0 m/s or higher, e.g. up to about 10.0 m/s.
In the outer section of the burner, argon is flown through opening 104 a, hydrogen through opening 105 a, argon through opening 106 a and oxygen through opening 107 a. In this case, oxygen is flown in a stoichometric ratio or preferably in slight excess with respect to hydrogen, the O2/H2 molar ratio being from about 1:2 to about 1:1 preferably from about 1:1.95 to about 1:1.75.
As previously mentioned, the hydrogen flowing from the outer section may also partially react with the excess of oxygen flowing from the inner section of the burner.
According to an alternative configuration shown in
The Applicant has further observed that by suitably redistributing the flow of forming glass particles before said flow impacts onto the target preform, it is possible to further increase the deposition rate of the burner. To this end, a multi-flame burner as disclosed previously is particularly suitable. In particular, the outlet of the quartz separating tube is suitably modified so to increase the deposition rate of the burner. The modification is such as to confer to the outlet of the quartz separating tube a cross-section having a major and a minor axis.
As a matter of fact, the Applicant has observed that for obtaining an optimal and homogeneous heating of the reacting glass precursor material, both the stream of glass precursor material and the surrounding inner flame shall preferably have a substantially circular geometry. On the other side, it has been observed that the deposition rate can be increased by increasing the dimensions of the flow of glass particles in a direction substantially perpendicular with respect to the longitudinal axis of the target preform.
As shown in
This redistribution of the stream of growing silica particles results in an increase of the deposition rate of the burner.
In order to effectively increase the deposition rate of the burner, the ratio between the major axis and the minor axis shall preferably be at least about 1.2 or higher. On the other side, in order to avoid an excessive modification of the geometry of the flow of glass particles (which may cause undesired turbulences in the flows of the burner) said ratio is preferably kept lower than about 2.5. Preferably, said ratio is from about 1.25 to about 1.8.
In addition, said major axis should be relatively smaller with respect to the initial diameter of the growing preform, in order to avoid excessive dispersion of silica particles. Preferably, said major axis is in a ratio of at least about 1:2 or higher with respect to the initial diameter of the growing preform, more preferably of at least about 1:2.5 or higher. On the other side, said major axis should be sufficiently large with respect to the final diameter of the preform, in order to effectively increase the deposition rate of the process.
In particular, the ratio between said major axis and the final diameter of the preform is preferably lower than about 1:7, preferably lower than about 1:6.
For instance, in a double burner overcladding deposition process as illustrated in
The burner of the present invention is particularly suitable for being used in the overcladding deposition of large diameter preforms, where the flow rate of the glass precursor material is typically kept higher than about 8 slm (standard liter per minute), in particular at about 10 slm or higher.
The so obtained preform is then heated into a furnace and collapsed to obtained a final preform of about 60-80 mm diameter, which is then drawn into an optical fiber according to conventional techniques.
While a burner according to the present invention can advantageously be used in the above process for depositing the overcladding layer of the preform, in particular the outer overcladding portion (i.e. as burner 704), it will be appreciated that such a burner, when suitably dimensioned, can also be used for the deposition of the core and of the inner portion of the cladding.
For this experiment, a burner comprising eight co-axial metal pipes as shown in
A quartz glass tube has been inserted between the third and the fourth metal pipe for providing the flame confinement. The following table 1 indicates the relative internal (ID) and outer (OD) diameter of the annular ducts determined by the metal pipes; for the innermost duct 1 a, having a circular cross section, only the OD has been reported. The inner section of the burner is formed by pipes 1 to 3 (and corresponding ducts 1 a to 3 a), while the outer section of the burner is formed by pipes 4 to 8 (and corresponding ducts 4 a to 7 a)
The internal confining quartz glass tube, having a thickness of about 1.5 mm, an inner diameter of 28.4 mm and an outer diameter of 31.4, has been inserted into the annular clearance between pipes 3 and 4 (ID 27.4 mm, OD 33.6 mm). The lower portion of the glass tube has been wrapped with a Teflon® tape up to the outer diameter of the clearance, in order to maintain it in a fixed position.
An outer quartz glass tube having a thickness of about 2 mm has been further disposed around the outer metal pipe 8.
As shown in
The reactants employed and their relative flow rate and inlet speed are reported in the following table 2, where the innermost opening of the burner is identified with no. 1 a. Silica tetrachloride has been supplied by vaporizing the liquid material and feeding it at a temperature of about 80° C. through the central pipe, together with oxygen.
Under these conditions, a theoretical length of the reaction zone of about 100-120 mm has been calculated, according to the relationship previously illustrated.
The target preform was a rotating quartz tube of about 90 mm diameter and the burner (i.e. the upper end of the outer glass tube of the burner) has been kept at a distance of about 50 mm from the preform, with an inclination of about 12° with respect to the longitudinal axis of the preform.
The preform was translated upwardly at a speed of 168 mm/h and rotated at about 60 r.p.m.
The deposition was stopped when the preform reached a diameter of about 140-150 mm.
By increasing the protruding length of the inner confining quartz tube from the tips of the metal pipes, an increase in the deposition rate has been observed, as reported in the following table 3. The deposition rate reported in table 3 is normalized with respect to the deposition rate of a burner without separating quartz tube (length 0 mm).
From the results reported in the above table 3, it can be observed that a tube with a length of 87-107 mm provides a substantial increase in the deposition rate. When using the longer tube (127 mm), although a slight increase in the deposition rate has still been observed, the resulting preform showed cracks in the deposited soot, which indicates a not appropriate density value. This is possibly caused by the fact that the outlet of the separating tube was positioned too close to the target preform, thus concentrating the inner flame onto a too small surface of the preform.
Some other experiments have thus been carried out by positioning the burner further 40 mm away from the target soot, and the recipe has been maintained as per table 2. Corresponding to three different separating tube lengths of 107, 133 and 153 mm, the obtained normalised deposition rates were 1.81, 1.89 and 1.83, respectively.
At the end of the deposition process, no damages or deformation have been observed onto the metal pipes forming the outer flame of the burner.
For this experiment a burner having a configuration according to
Dimensions of ducts created by pipes 1-9 and the relative flow of materials is reported in tables 4 and 5, respectively.
The internal separating quartz glass tube, having a thickness of about 1.5 mm, has been inserted into the annular clearance between pipes 5 and 6.
An outer quartz glass tube having a thickness of about 2 mm has been further disposed around tube the outer metal pipe 9.
In this experiment, the tips of pipes 6 to 9, forming the outer section of the burner, were spaced forwardly of about 53 mm from the tips of the pipes 1 to 5, forming the inner section of the burner.
The inner quartz separating tube was prolonged for about 70 mm from the tips of the pipes of the outer section, having thus a total length of about 123 mm from the tips of the pipes of the inner section.
The target preform was a rotating quartz tube of about 90 mm diameter and the burner has been kept at a distance of about 90 mm from the preform, with an inclination of about 12° with respect to the longitudinal axis of the preform.
The preform was translated upwardly at a speed of 168 mm/hr and rotated at about 60 r.p.m.
The deposition was stopped when the preform reached a diameter of about 140-150 mm.
The above burner has then been modified by conferring an elliptical cross-section to the terminal portion of the separating quartz tube, as shown in
The burner has then been positioned similarly to the previous test, with the major axis of the elliptical cross-section of the quartz tube laying on a plane substantially perpendicular to the longitudinal axis of the target preform. The process conditions were as previously described.
A normalized deposition rate (with respect to the value obtained with the circular cross-section burner) of about 1.08 was obtained.
As a comparative experiment, the above burner has been rotated of 90° with respect to its own longitudinal axis, so to exchange the relative positions of the major and of the minor axis. In this case, a deposition rate of about 0.76.
As shown by the above results, it is thus possible to increase the deposition rate of a burner according to the invention by suitably modifying the cross-section of the outlet of the separating quartz tube.